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VIPER53 数据表(PDF) 18 Page - STMicroelectronics |
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VIPER53 数据表(HTML) 18 Page - STMicroelectronics |
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18 / 24 page ![]() VIPer53DIP / VIPer53SP 18/24 in the current mode section. A zero due to the RCOMP-CCOMP network is set at the same value as the maximum load RL2 pole. The total transfer function is shown as F(s).G(s) at the bottom of figure 20. For maximum load (plain line), the load pole is exactly compensated by the zero of the error amplifier, and the result is a perfect first order decreasing slope until it reaches the zero of the output capacitor ESR. The error amplifier cut off then prevents definitely any further spurious noise or resonance from disturbing the regulation loop. The point where the complete transfer function has a unity gain is known as the regulation bandwidth and has a double interest: – The higher it is the faster will be the reaction to an eventual load change, and the smaller will be the output voltage change. – The phase shift in the complete system at this point has to be less than 135 ° to ensure a good stability. Generally, a first order gives 90 ° of phase shift, and 180 ° for a second order. In figure 20, the unity gain is reached in a first order slope, so the stability is ensured. The dynamic load regulation is improved by increasing the regulation bandwidth, but some limitations have to be respected: As the transfer function above the zero due the capacitor ESR is not reliable (The ESR itself is not well specified, and other parasitic effects may take place), the bandwidth should always be lower than the minimum of FC and ESR zero. As the highest bandwidth is obtained with the highest output power (Plain line with RL2 load in figure 20), the above criteria will be checked for this condition and allows to define the value of RCOMP, as the error amplifier gain depends only on this value for this frequency range. The following formula can be derived: With: And: : The lowest load gives another condition for stability: The frequency FBW1 must not encounter the second order slope generated by the load pole and the integrator part of the error amplifier. This condition can be met by adjusting the CCOMP value: With: The above formula gives a minimum value for CCOMP. It can be then increased to provide a natural soft start function as this capacitor is charged by the error amplifier current capacity ICOMPhi at start-up. Figure 20: Complete Converter Transfer Function G(S) F FC F F F(S) F(S).G(S) 1 π R L 1 C OUT ⋅⋅ ---------------------------------------- 1 π R L 2 C OUT ⋅⋅ ---------------------------------------- 1 2 π ESR C OUT ⋅⋅ ⋅ ------------------------------------------------ 1 2 π R COM P C CO M P ⋅⋅ ⋅ ---------------------------------------------------------------- FBW2 FBW1 1 1 1 3.2 P MA X P OU T 2 -------------------- ⋅ 3.2 P MAX P OUT1 -------------------- ⋅ Gm R COM P ⋅ R COMP P OUT2 P MAX ----------------- F BW 2 RL2 COUT ⋅⋅ Gm ------------------------------------------------ ⋅ = P OUT2 V OUT 2 R L2 -------------- = P MAX 1 2 --- L P I LIM 2 F SW ⋅⋅ ⋅ = C COMP R L1 COUT ⋅ 6.3 Gm R COMP 2 ⋅⋅ --------------------------------------------- P OUT1 P MAX ----------------- ⋅ > P OUT1 V OUT 2 R L1 -------------- = |
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